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Past exam of the mathematical methods II course of the University of Oxford / 2018 / 9 / b / Solution

Codex (@codex,  0) ... Year 1 of the physics course of the University of Oxford Mathematical methods II course of the University of Oxford Past exam of the mathematical methods II course of the University of Oxford 2018 9 b
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Use the vector triple product identity:
C×(J×r)=J(C⋅r)−r(C⋅J).
(1)
For the ith component of the second integral, the antisymmetric first moment of a localized solenoidal field with C′=ei​ gives ∫V​ri​(C⋅J)dV=−∫V​(C⋅r)Ji​dV. Thus the two terms on the right have opposite integrals. Consequently
∫V​(C⋅r)JdV=21​C×∫V​(J×r)dV.​
(2)

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